Heavy axial-vector structures bbc‾c‾
The fully heavy axial-vector diquark-antidiquark structures bbc‾c‾ are explored by means of the QCD sum rule method. They are modeled as four-quark mesons T1 and T2 composed of bTCσμνγ5b, c‾γνCc‾T and bTCγμγ5b, c‾Cc‾T diquarks, respectively. The spectroscopic parameters of the tetraquarks T1 and T2...
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Format: | Article |
Language: | English |
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Elsevier
2024-04-01
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Series: | Physics Letters B |
Online Access: | http://www.sciencedirect.com/science/article/pii/S0370269324001205 |
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author | S.S. Agaev K. Azizi H. Sundu |
author_facet | S.S. Agaev K. Azizi H. Sundu |
author_sort | S.S. Agaev |
collection | DOAJ |
description | The fully heavy axial-vector diquark-antidiquark structures bbc‾c‾ are explored by means of the QCD sum rule method. They are modeled as four-quark mesons T1 and T2 composed of bTCσμνγ5b, c‾γνCc‾T and bTCγμγ5b, c‾Cc‾T diquarks, respectively. The spectroscopic parameters of the tetraquarks T1 and T2 are determined in the context of the QCD two-point sum rule method. Results obtained for masses of these states m1=(12715±86)MeV and m2=(13383±92)MeV are used to fix their strong decay channels. The full width Γ(T1) of the diquark-antidiquark state T1 is estimated by considering the processes T1→Bc−Bc⁎− and T1→Bc⁎−Bc⁎−. The decays to mesons Bc−Bc⁎−, Bc−(2S)Bc⁎− and Bc⁎−Bc⁎− are employed to evaluate Γ(T2). Results obtained for the widths Γ(T1)=(44.3±8.8)MeV and Γ(T2)=(82.5±13.7)MeV of these tetraquarks in conjunction with their masses are useful for future experimental studies of fully heavy resonances. |
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id | doaj.art-03f31f925cfa42d28c5bd6c59c8d6d4f |
institution | Directory Open Access Journal |
issn | 0370-2693 |
language | English |
last_indexed | 2024-04-24T13:11:18Z |
publishDate | 2024-04-01 |
publisher | Elsevier |
record_format | Article |
series | Physics Letters B |
spelling | doaj.art-03f31f925cfa42d28c5bd6c59c8d6d4f2024-04-05T04:39:45ZengElsevierPhysics Letters B0370-26932024-04-01851138562Heavy axial-vector structures bbc‾c‾S.S. Agaev0K. Azizi1H. Sundu2Institute for Physical Problems, Baku State University, Az–1148 Baku, AzerbaijanDepartment of Physics, University of Tehran, North Karegar Avenue, Tehran 14395-547, Iran; Department of Physics, Doǧuş University, Dudullu-Ümraniye, 34775 Istanbul, Türkiye; Corresponding author.Department of Physics Engineering, Istanbul Medeniyet University, 34700 Istanbul, TürkiyeThe fully heavy axial-vector diquark-antidiquark structures bbc‾c‾ are explored by means of the QCD sum rule method. They are modeled as four-quark mesons T1 and T2 composed of bTCσμνγ5b, c‾γνCc‾T and bTCγμγ5b, c‾Cc‾T diquarks, respectively. The spectroscopic parameters of the tetraquarks T1 and T2 are determined in the context of the QCD two-point sum rule method. Results obtained for masses of these states m1=(12715±86)MeV and m2=(13383±92)MeV are used to fix their strong decay channels. The full width Γ(T1) of the diquark-antidiquark state T1 is estimated by considering the processes T1→Bc−Bc⁎− and T1→Bc⁎−Bc⁎−. The decays to mesons Bc−Bc⁎−, Bc−(2S)Bc⁎− and Bc⁎−Bc⁎− are employed to evaluate Γ(T2). Results obtained for the widths Γ(T1)=(44.3±8.8)MeV and Γ(T2)=(82.5±13.7)MeV of these tetraquarks in conjunction with their masses are useful for future experimental studies of fully heavy resonances.http://www.sciencedirect.com/science/article/pii/S0370269324001205 |
spellingShingle | S.S. Agaev K. Azizi H. Sundu Heavy axial-vector structures bbc‾c‾ Physics Letters B |
title | Heavy axial-vector structures bbc‾c‾ |
title_full | Heavy axial-vector structures bbc‾c‾ |
title_fullStr | Heavy axial-vector structures bbc‾c‾ |
title_full_unstemmed | Heavy axial-vector structures bbc‾c‾ |
title_short | Heavy axial-vector structures bbc‾c‾ |
title_sort | heavy axial vector structures bbc‾c‾ |
url | http://www.sciencedirect.com/science/article/pii/S0370269324001205 |
work_keys_str_mv | AT ssagaev heavyaxialvectorstructuresbbcc AT kazizi heavyaxialvectorstructuresbbcc AT hsundu heavyaxialvectorstructuresbbcc |